First Law for Open Systems
Beginning with the general balance equation, we can develop an
expression for the open system energy balance. For now, lets work with
a SISO (single input, single output) system. We can always add the
extra terms for extra inlet and outlet streams if needed.
Each element of fluid possesses internal, kinetic, and potential energy,
so:
Next, look at the work term. Recall that there are three types of work:
- boundary movement work
- flow work
- shaft work
Just as we did for the open system mass balance, we usually do our best
to set up the system with fixed volume; therefore, there will not be any
boundary movement work, and the work term can be written:
Notice how the sign convention applies -- work is done on the system
(negative) to move fluid into the system, work is done by the system
(positive) to move flow out of the system.
When everything is assembled, we apply the definition of enthalpy to
get:
This is equivalent to equation 6.7 in the text and is
important. This is a very general form of the open
system energy balance, and will be the starting point for developments
in the next several classes.
References:
- Cengel, Y.A. and M.A. Boles, Thermodynamics: An Engineering
Approach (3rd ed.), WCB McGraw-Hill, 1998, p. 197-200.
- Sonntag, R.E., C. Borgnakke, and G.J. Van Wylen, Fundamentals
of Thermodynamics (6th ed.), John Wiley, 2003, p. 165-67.
- Sonntag, R.E., C. Borgnakke, and G.J. Van Wylen, Fundamentals
of Thermodynamics (5th ed.), John Wiley, 1998, p. 143-45.
R.M. Price
Original: 5/1/2000
Modified: 5/25/2000; 10/18/2003
Copyright 2004 by R.M. Price -- All Rights Reserved